More on the renormalization of the horizon function of the Gribov-Zwanziger action and the Kugo-Ojima Green function(s)
arXiv:1001.3103 · doi:10.1140/epjc/s10052-010-1304-8
Abstract
In this paper we provide strong evidence that there is no ambiguity in the choice of the horizon function underlying the Gribov-Zwanziger action. We show that there is only one correct possibility which is determined by the requirement of multiplicative renormalizability. As a consequence, this means that relations derived from other horizon functions cannot be given a consistent interpretation in terms of a local and renormalizable quantum field theory. In addition, we also discuss that the Kugo-Ojima functions and can only be defined after renormalization of the underlying Green function(s).
16 pages, some typo's corrected
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- Locating the Gribov horizon
- Brout-Englert-Higgs physics: From foundations to phenomenology
- QCD Running Couplings and Effective Charges
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- More on the non-perturbative Gribov-Zwanziger quantization of linear covariant gauges
- A remark on the BRST symmetry in the Gribov-Zwanziger theory
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- Accessing the topological susceptibility via the Gribov horizon
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- On Gauge Independence for Gauge Models with Soft Breaking of BRST Symmetry
- Comments on the compatibility of thermodynamic equilibrium conditions with lattice propagators
- Local QCD Action at Finite Temperature
- The gap equations of background field invariant Refined Gribov-Zwanziger action proposals and the deconfinement transition
- A mass-deformed BLG theory in Gribov-Zwanziger framework
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- Confining Potentials
- A modification of Faddeev-Popov approach free from Gribov ambiguity